[0001] This invention relates to a viewing angle colour sensitive lighting accessory.
[0002] Home lighting may be used for decoration, such as, for example, lighted, coloured,
ceiling, wall or floor panels. The lighting may be solely decorative or may also be
provided to light an area.
[0003] Other lighting devices are provided for instructional purposes, such as, for example,
lighted, coloured advertising panels or warning notices.
[0004] Whether these known types of lighting devices are for decoration or instructional
purposes they can only transmit a light of a particular colouration when viewed at
any angle within that of the emitted light.
[0005] There is a need for a lighting accessory which is viewing angle sensitive, that is,
the light viewed emanating from the accessory is dependant upon the angle at which
the accessory is viewed. Such an accessory could be used as an attractive adornment
or an attention attracting instructional device.
[0006] As an example, it has already been proposed in Canadian Patent No. 142,358, dated
August 13, 1912, "Lamps for Matching Colors by Artificial Light", M. Weety, to provide
a light fixture with blue and green glass filters to modify the light so as to cause
it to give the same effect as daylight.
[0007] It has also been proposed in Canadian Patent No. 318,588, dated January 5, 1932,
"Artificial daylight lighting units" , D.W. King, to provide an electric lamp with
a " daylight" vari-coloured reflector or shade and a transparent screen of blue colour
arranged around the lower part of the lamp, the relative disposition of the screen
and shade being such that no light is given out from the lamp which is not either
reflected from the shade or transmitted through the screen.
[0008] It has further been proposed in Canadian Patent No. 238,091, dated July 6, 1920,
"Artificial Illumination" , G.H. Sheringham, to provide an ordinary incandescent lamp
with a reflector or shade which is suitably coloured on its reflecting surface so
as to act as a reflecting compensating member. An ordinary incandescent lamp usually
alters the hue of such colours as violet, blue and green and the compensating member
used in combination with such lamps would be coloured with two or more colours in
such proportion and concentration as to absorb a suitable proportion of the excessive
rays while reflecting the feeble rays present in the spectrum of the lamp light. In
the case when the resultant light is partly direct and partly reflected, it is necessary
in order to counterbalance as far as possible the unavoidable lack of balance in the
quality of the direct light, to cause the reflected light to be compensatingly out
of balance in the reverse direction. In other words the proportion and concentration
of the colours on the reflector are so chosen that the reflected light has, in comparison
with daylight, a greater relative proportion of the rays which are feeble in the direct
light. The colours may be arranged upon the reflecting surface of the shade in suitable
lines or patterns and the meeting edges of the different colours may be serrated.
[0009] Previous attempts to simulate daylight in an artificial manner have failed to do
so because, under clear sky conditions, natural outdoor illumination has an important
property that has been overlooked in that there is a marked variation of colour with
angle. The direct rays of sunlight have a slightly yellow tint, while the illumination
at peripheral angles has the characteristic blue colour of the sky. The result is
that objects which are not illuminated directly by sunlight appear more blue than
they otherwise would and a good example of this is that shadows on a sunny day are
blue.
[0010] The fact that most people are not directly aware of this phenomenon is a result of
the accommodation ability of their visual perception system. In effect, they automatically
take into account the colour of ambient light when they perceive the colour of an
object. Nevertheless, many people would agree that clear sky illumination with its
" blue shadow" effect has a different quality than, for example, cloudy sky illumination
and many find the former preferable.
[0011] At present, most artificial interior illumination systems do not incorporate a variation
of colour with angle, and as a result they produce lighting similar to that of a cloudy
sky.
[0012] There is a need for a lighting accessory that more realistically simulates clear
sky conditions than known lighting devices in that a marked variation of colour with
angle is perceived in a similar manner to clear sky conditions, and such an accessory
can be provided by one which is viewing angle sensitive as previously defined herein.
[0013] In Canadian Patent No. 944,987, dated April 9, 1974, " Optical Interference Authenticating
Means" , K.M. Baird, J.A. Dobrowolski, P.D. Carman and A.J. Waldorf, it has been proposed
in one embodiment to provide an optical interference authenticating means comprising
a number of optical interference multilayer coatings each having spectral transmittance
characteristics which vary with the angle of incidence of light thereon. The multilayer
coatings form a covering over a transparent portion of a document to be authenticated
so that the spectral transmittance characteristics may be viewed from the opposite
side of the multilayer coatings, from that which the light beam impinges upon them,
as a viewing angle sensitive colour change.
[0014] While the colour change effect taught by Canadian Patent No. 944,987 has been shown
to be readily observable when closely viewing the multilayer coatings covering a small,
transparent area of a document to be authenticated, it could not be deduced from this
that the same effect could be readily observed from the distances that, for example,
overhead lighting fixtures are viewed by an observer.
[0015] According to the present invention, there is provided a viewing angle colour sensitive,
lighting accessory, comprising:
(a) a sheet member for attachment to a light emitting source and capable of transmitting
visible light therefrom forwardly towards an area from which transmitted light is
to be perceived, and
(b) at least one optical interference multilayer coating on the sheet member, the
material for each layer of the multilayers being selected so that the coating has
different spectral transmittance characteristics at different angles of incidence
of the visible light thereto so that light thereof of a particular colouration will
be perceived transmitted through the coating at at least one range of viewing angles
thereto, and
(c) securing means for securing the sheet member to the light emitting source.
[0016] Preferably the securing means is for removably securing the sheet member to the light
source.
[0017] In some embodiments of the present invention there is provided an electromagnetic
radiation reflector securing the sheet member and extending rearwardly there behind
around the light emitting source which is mounted therein, so that visible light will
be reflected by the reflector forwardly towards the area from which light is to be
perceived.
[0018] In yet other embodiments of the present invention, each coating is of a material
selected from the group consisting of cryolite, NaF, LiF, MyF
2, SiO
2, ThFu, LaF
3, NdF
3, CeF,, GeO
2, ThO
2, AP
2O
3, MgO, PbF,, CeO
2 , Sb
2= O
3 , HfO
2 , Bi
2O
3, La
2O
3, SC
2O
3, Nd
2O
3 , Ta
2O
5, SiN, ZrO
2, ZnS, TiO
2, Ag, A1, Au, Cu, Cr, Ge, Ni, NiCr, Si, Rh. It is conceivable that other materials
with similar properties might be employed too.
[0019] The thickness of each coating is normally within one or two orders of magnitude of
O.lum.
[0020] In the accompanying drawings which illustrate, by way of example, embodiments of
the present invention,
Figure 1 is an end view of a viewing angle sensitive, lighting accessory using incandescent
light sources with a portion of an end reflector wall removed to expose the interior,
Figure 2 is a sectional end view of a different, viewing angle sensitive, lighting
accessory to that shown in Figure 1, using a prism light guide as a light source,
Figures 3 to 5 are graphs showing the calculated spectral transmittance values of
an optical interference multilayer coating for light incident thereon at angles of
0°, 45° and 75° respectively,
Figure 6 depicts calculated and measured CIE chromaticity coordinate differences between
normal transmittance angle and various other transmittance angles, for a Prism Light
Guide luminaire provided with an optical interference multilayer coating on its emitting
surface.
[0021] In Figure 1 there is shown a viewing angle sensitive, lighting accessory, comprising:
(a) a sheet member 1 for attachment to a light emitting source 2 and capable of transmitting
visible light therefrom forwardly in the directions of arrows A to D towards an area
from which light is to be perceived,
(b) at least one optical interference multilayer coating 3 on the sheet member 1,
the material and thickness for each layer of the multilayer being selected so that
the coating has different spectral reflectance and spectral transmittance characteristics
and, if desired, states of polarization at different angles of incidence of the visible
light thereto so that light of a particular colouration and, if desired, polarization
will be perceived transmitted through the coating at at least one range of viewing
angles thereto, and
(c) securing means, in the form of flanges 4 and 6.
[0022] The light emitting source 2 is an incandescent light fixture.
[0023] An electromagnetic radiation reflector, generally designated 5 and having a highly
reflective interior, comprises an inverted U-shaped casing 8 which extends rearwardly
behind the sheet member 1 so that electromagnetic radiation will be reflected by the
reflector 5 forwardly towards the area from which light is to be perceived. The flanges
4 and 6 are attached to the sides of the inverted U-shaped casing 8 and extend inwardly
therefrom. The reflector 5 has end walls 10 and 12. The light emitting source 2 is
mounted in the reflector 5. The sheet member 1, with the multilayer coating 3 thereon,
is secured on the flanges 4 and 6 by being slid on them beneath the end wall 10 until
the sheet member 1 butts against the end wall 12. Thus the sheet member 1 is removably
secured to the light emitting source 2.
[0024] In operation, the light perceived from the accessory along the viewing angle of arrow
A will be of a particular colouration changing to a different colouration along the
viewing angle of arrow B to yet another colouration along the viewing angle C and
back again through the same colourations along the viewing angles D and E. How this
is achieved will be described later.
[0025] The materials for the optical interference coatings can be selected so that the multilayer
coating 3 has the property that the significant fraction of the electromagnetic radiation
which is not transmitted through it is reflected back towards the highly reflective
interior of the reflector 5 to be reflected back therefrom so that it has another
opportunity to be transmitted through the multilayer coating.
[0026] In Figure 2, similar parts to those shown in Figure 1 are given the same reference
numerals and the previous description is relied upon to describe them.
[0027] In Figure 2, a light emitting source 14 is provided comprising a light guide of the
type described and claimed in United States Patent No. 4,260,220, dated April 7, 1981,
" Prism Light Guide Having Surfaces which are in Octature" , L.A. Whitehead. The light
guide comprises a longitudinal, hollow structure made of transparent or translucent
material, e.g. acrylic plastic or optically clear glass, and has planar inner and
outer surfaces which are in " octature" . An inverted U-shaped outer, protective casing
16 is provided having flanges 18 and 20 securing the sheet member 1 with the multilayer
coating 3 thereon in the same manner as the flanges 4 and 6 in Figure 1.
[0028] The light that is provided at one or both ends of the light guide may, for example,
be a reflected beam of sunlight by day, when available, and an artificial beam of
light at other times. In some embodiments sunlight, when available, may be reflected
into one end of the light guide and artificial light beamed in the other end thereof
at other times.
[0029] The lighting device shown in Figure 2 functions in the same manner as the lighting
device shown in Figure 1.
[0030] Under typical clear sky conditions, at mid-latitude and mid-day, typical CIE chromaticity
coordinates for the light coming directly from the sun are (.335, .340). In comparison,
typical coordinates of the blue sky are (.275, .285).
[0031] The following is an example of artifically simulating this chromaticity difference:
If a reflected beam of sunlight is directed along the light guide shown in Figure
2, then the simulation of clear sky daylight illumination is achieved by the coatings
of the optical interference multilayer coating 3 being chosen so as to act as a long
wavelength cut-off filter whose normal transition wavelength is just outside the visible
spectral range, and which shifts towards shorter wavelengths with a more acute viewing
angle of incidence to the optical interference multilayer coating 3. The design parameters
for one such an optical interference multilayer coating 3 are set out below. Many
other designs with similar performance could be produced by known techniques.
[0032] The transmittance T and reflectance R of a non-absorbing optical interference multilayer
coating 3 consisting of N layers can be expressed in terms of the refractive indices
n
o, n of the incident and substrate media and of the elements of the product matrix
M given by

Here

[0033] For a film at non-normal angle of incidence ε
j and u. are the effective optical phase thickness and effective refractive index,
given by and


[0034] The angle φ is the angle of refraction within the j-th film. It is related to the
angle of incidence 0 by Snell's law:

where n
j is the refractive index of the j-th layer.
[0035] It follows from (3) that with increasing angle of incidence the effective phase thicknesses
of the layers get smaller, and therefore the spectral features of the multilayer are
displaced towards shorter wavelengths. The effective indices get smaller or larger,
for radiation polarized parallel or perpendicular, respectively, to the plane of incidence
(4). At larger angles this results in marked polarization splitting and a distortion
of the normal incidence spectral features. But the human eye does not distinguish
light of different polarizations and perceives only the average of the two components,

These are therefore the quantities that have to be optimized in the design process.
[0036] Empirical results with many different all-dielectric optical interference multilayer
costings 3 has shown that, at least for smaller angles of incidence (O , 30°), the
shift of the coarse spectral features is proportional to cost, where

is given by

where the average refractive index n of the optical interference multilayer coating
3 is defined as follows:

[0037] It will be seen from (6) that n will determine the rate at whith the coarse spectral
features will shift with angle. There will be thus an optimal valme for n. Even within
this constraint there are many different ways of designing a long wavelength cut-off
filter. However, it is desirable that the resulting optical interference multilayer
coating 3 be rugged and be as economical to produce as possible. It is a well-known
fact that low transmissions in the rejection region are achieved with the least number
of optically non-absorbing coatings with quarter-wave stacks composed of two materials
with refractive indices whose ratio is as high as possible. It was therefore decided
to use quarter-wave stacks as a starting point in an automatic thin film synthesis
program. SiO
2 is the hard coating material with the lowest refractive index (1.45), and a suitable
high refractive index material is ZrO
2 which yields an acceptable refractive index ratio and mean refractive index. Unfortunately,
with this pair of materials at high angles of incidence a transmission band appears
in the red part of the spectrum. Should this be undesirable, a more complicated optical
interference multilayer coating 3 can be designed.
[0038] The above approach was used to numerically design several optical interference multilayer
coatings 3. The results given below are for a fifteen-layer system whose construction
parameters are given in the following table.
[0039] As can be seen, the polarization of the transmitted light increases strongly with
the angle of viewing. At larger angles the transmittance for light polarized parallel
to the plane of viewing is significantly larger than that for light polarized perpendicular
to that plane. When the surface is mounted horizontally, this result serves to simulate
the polarization characteristics of natural sky light in which peripheral rays are
substantially polarized.

[0040] The calculated spectrac transmittance of this optical interference multilayer coating
at 0°, 45°, and 75° incidence are given in Figures 3 to 5 respectively, where T is
the transmittance and λ is the wavelength in µm. In these figures, designates light
polarized parallel to the plane of incidence, and 1 designates light polarized perpendicular
to the plane of incidence.
[0041] The corresponding calculated CIE coordinate differences Ax, Ay between normal incidence
transmittance and transmittance at other angles are plotted in a dashed line in Figure
6. A source C illumination was assumed in the calculations.
[0042] The coatings were deposited onto a 0.004" thick polyester film substrate in a high
vacuum box coater. An electron beam gun was used to deposit the coatings. The most
sensitive wavelength method was used to monitor the deposition process. The measured
normal incidence spectral transmittance of the resulting multilayer corresponded to
those shown in Figure 3.
[0043] The coated polyester film was mounted on a short section of a light guide of the
type shown in Figure 2, and a portable colourimeter made by Minolta was used to measure
the colour of the transmitted radiation. The results are shown by continuous line
in Figure 6. There is a discrepancy between the calculated and measured colour differences,
which is believed to be caused by the fact that the spectral energy distribution of
the light incident on the polyester film was subtly different than the theoretical
source C used for the calculation. Nevertheless, there is qualitative agreement between
theory and experiment. The CIE coordinates of the same light guide, but without the
angle sensitive lighting accessory, were measured and were found to be substantially
independent of angle, as expected. These results show a performance that is a significant
step towards simulating the difference in colour between blue sky and direct sunlight,
which is also depicted (point A) in Figure 6.
[0044] The experimental design demonstrated that it is possible to simulate clear sky illumination
with direct sunlight which is, for example, channelled through a light guide of the
type shown in Figure 2, and a specially designed viewing angle sensitive, optical
interference multilayer coating. The same design criteria can be applied to viewing
angle sensitive, light accessories based on artificial light sources. For example,
it is a relatively easy matter in addition to modify the normal incidence transmittance
of the multilayer coating to adjust the light emissions of incandescent sources to
clear sky daylight illumination.
[0045] For the techniques described in this paper to be practical, equipment must exist
for the accurate mass production of such complicated multilayer structures at low
per-unit area cost. Work on such facilities is well advanced at several places.
[0046] Lighting fixtures according to the present invention may be used for decorative effects,
instructional purposes, or for a source of illumination in addition to the decorative
effects or instructional purposes.
[0047] Light fixtures according to the present invention may be used overhead, laterally
spaced from or at a lower level than the observer. It is clear that for these applications
many different angle sensitive, lighting accessories can be designed and constructed
with other, interesting colour changes of the perceived light.
[0048] In some embodiments of the present invention the optical interference multilayer
coating is angle sensitive with respect to polarization. It will be understood that
in order for the change in polarization with angle to be observed, it is necessary
for the light from the accessory to be viewed with the aid of a light polarizing device.
[0049] The coatings of the multilayer coating 3 may be made of non-absorbing materials such
as, for example, cryolite, NaF, LiF, MyF
2 , SiO
2 , ThFu, LaF,, hdF
3 , CeF,, GeO
2 , ThO
2 , Al
2O
3, MgO, PbF
2, CeO
2, Sb
2O
3, HfO
2, Bi
2O
3, La
2O
3, SC
2O
3, Nd
2O
3, Ta
2O
5, SiN, ZrO
2, ZnS, TiO
2, Ag, Al, Au, Cu, Cr, Ge, Ni, NiCo, Si, Rh, or any other materials that form satisfactory
layers or coatings. The thicknesses of the coatings will normally be within one or
two orders of magnitude of 0.1 µm.
[0050] It will be appreciated that it is within the scope of the present invention for:
i) the light source to be in the form of a light guide
ii) the colour sensitive light accessory to cause a variation of colour with angle
which substantially simulates the variation found with clear sky illumination, and
iii) the accessory to substantially simulate the variation of polarization with angle
found with clear sky illumination.
1. A viewing angle colour sensitive, lighting accessory, comprising:
(a) a sheet member for attachment to a light emitting source and capable of transmitting
visible light therefrom forwardly towards an area from which transmitted light is
to be perceived, and
(b) at least one optical interference multilayer coating on the sheet member, the
material and thickness for each layer of the multilayers being selected so that the
coating has different spectral transmittance characteristics at different angles of
incidence of the visible light thereto so that light thereof of a particular colouration
will be perceived transmitted through the coating at at least one range of viewing
angles thereto, and
(c) securing means for securing the sheet member to the light emitting source.
2. An accessory according to Claim 1, wherein the securing means is for removably
securing the sheet member to the light source.
3. An accessory according to Claim 1 or 2, wherein an electromagnetic radiation reflector
is provided securing the sheet member and extending rearwardly therebehind and around
the light emitting source, which is mounted therein, so that visible light will be
reflected by the reflector forwardly towards the area from which light is to be perceived.
4. An accessory according to Claim 1, wherein the light source is a light guide.
5. An accessory according to Claim 1, wherein each coating is of a material selected
from the group consisting of cryolite, NaF, LiF, MyF,, SiO2, ThFu, LaF3, NdF3, CeF3, GeO2, ThO2 , Al2O3 , MgO, PbF2, CeO2 , Sb2 O3 , HfO2, Bi2O3, La2O3, SC2O3, Nd2O3, Ta2O5, SiN, ZrO,, ZnS, TiO2, Ag, Al, Au, Cu, Cr, Ge, NiCr, Si, and Rh.
6. An accessory according to Claim 5, wherein the thickness of each coating is within
one or two orders of magnitude of 0.1 µm.
7. An accessory according to Claim 3 and Claim 4, wherein the colour sensitive light
accessory causes a variation of colour with angle which substantially simulates the
variation found with clear sky illumination.
8. An accessory according to Claim 7, wherein the accessory also substantially simulates
the variation of polarization with angle which is found with clear sky illumination.